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  • CERN-LHC. This paper presents a measurement of jet fragmentation functions in 0.49 nb−1 of Pb+Pb collisions and 25 pb−1 of pp collisions at sNN=5.02 TeV collected in 2015 with the ATLAS detector at the LHC. These measurements provide insight into the jet quenching process in the quark-gluon plasma created in the aftermath of ultrarelativistic collisions between two nuclei. The modifications to the jet fragmentation functions are quantified by dividing the measurements in Pb+Pb collisions by baseline measurements in pp collisions. This ratio is studied as a function of the transverse momentum of the jet, the jet rapidity, and the centrality of the collision. In both collision systems, the jet fragmentation functions are measured for jets with transverse momentum between 126 and 398 GeV and with an absolute value of jet rapidity less than 2.1. An enhancement of particles carrying a small fraction of the jet momentum is observed, which increases with centrality and with increasing jet transverse momentum. Yields of particles carrying a very large fraction of the jet momentum are also observed to be enhanced. Between these two enhancements of the fragmentation functions a suppression of particles carrying an intermediate fraction of the jet momentum is observed in Pb+Pb collisions. A small dependence of the modifications on jet rapidity is observed. The ratio of the D(pT) in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.0 < eta < 2.1.

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    HEPData
    Dataset . 2020
    Data sources: Datacite
    HEPData
    Dataset . 2019
    Data sources: Datacite
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      HEPData
      Dataset . 2020
      Data sources: Datacite
      HEPData
      Dataset . 2019
      Data sources: Datacite
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  • Authors: Weinstabl, Harald; Suhartono, Marcel; Qureshi, Zafar; Lautens, Mark;

    Related Article: Zafar Qureshi, Harald Weinstabl, Marcel Suhartono, Hongqiang Lui, Pierre Thesmar, Mark Lautens|2014|Eur.J.Org.Chem.|2014|4053|doi:10.1002/ejoc.201402218 Related Article: Harald Weinstabl, Marcel Suhartono, Zafar Qureshi and Mark Lautens|2013|Angew.Chem.,Int.Ed.|52|5305|doi:10.1002/anie.201302327

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  • image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/

    Additional file7: Table S18. DNAmeQTL analysis for the loci significantly associated with DNAme-based XCI status calls. See additional files. These loci were independently tested as DNAmeQTLs in females and males, with some columns color coded based on sex (pink female, light blue male). There are also columns with the median and mean DNAme value at the gene’s island for samples with the reference or alternate allele at that loci; these columns are color coded based on whether the allele is in the range to escape from XCI (DNAme<0.01, blue) or in the range to be subject to XCI (DNAme>0.15, orange). There are mean and median columns for both males and females, but only the female columns are color coded based on XCI status. There are boxes around the genes with female median values with one allele in the range to escape XCI and the other allele in the range to be subject to XCI.

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    Dataset . 2022
    License: CC BY
    Data sources: Datacite
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    Dataset . 2022
    License: CC BY
    Data sources: Datacite
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      figshare
      Dataset . 2022
      License: CC BY
      Data sources: Datacite
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      figshare
      Dataset . 2022
      License: CC BY
      Data sources: Datacite
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  • Authors: Choing, Stephanie N.; Francis, Aaron J.; Clendenning, Graham; Schuurman, Michael S.; +4 Authors

    An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures. Related Article: Stephanie N. Choing, Aaron J. Francis, Graham Clendenning, Michael S. Schuurman, Roger D. Sommer, Isaac Tamblyn, Walter W. Weare, Tanja Cuk|2015|J.Phys.Chem.C|119|17029|doi:10.1021/acs.jpcc.5b00513

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    Table S1. Detrital zircon U-Pb isotopic analyses of sandstones from the Duoni Formation.Table S2. Detrital Cr-spinel geochemical compositions of sandstones from the Duoni Formation. THIS DATASET IS ARCHIVED AT DANS/EASY, BUT NOT ACCESSIBLE HERE. TO VIEW A LIST OF FILES AND ACCESS THE FILES IN THIS DATASET CLICK ON THE DOI-LINK ABOVE

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    DANS-EASY
    Dataset . 2020
    Data sources: B2FIND
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    Mendeley Data
    Dataset . 2020
    License: CC 0
    Data sources: Mendeley Data
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    Mendeley Data
    Dataset . 2020
    License: CC 0
    Data sources: Datacite
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    Mendeley Data
    Dataset . 2020
    License: CC 0
    Data sources: Mendeley Data
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    Mendeley Data; NARCIS
    Dataset . 2020
    License: CC 0
    Data sources: Datacite; NARCIS
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      DANS-EASY
      Dataset . 2020
      Data sources: B2FIND
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      Mendeley Data
      Dataset . 2020
      License: CC 0
      Data sources: Mendeley Data
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      Mendeley Data
      Dataset . 2020
      License: CC 0
      Data sources: Datacite
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      Mendeley Data
      Dataset . 2020
      License: CC 0
      Data sources: Mendeley Data
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      Mendeley Data; NARCIS
      Dataset . 2020
      License: CC 0
      Data sources: Datacite; NARCIS
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    Authors: Lynch, Karlene H; Stothard, Paul; Dennis, Jonathan J;

    Abstract Background The Burkholderia cepacia complex (BCC) is comprised of at least seventeen Gram-negative species that cause infections in cystic fibrosis patients. Because BCC bacteria are broadly antibiotic resistant, phage therapy is currently being investigated as a possible alternative treatment for these infections. The purpose of our study was to sequence and characterize three novel BCC-specific phages: KS5 (vB_BceM-KS5 or vB_BmuZ-ATCC 17616), KS14 (vB_BceM-KS14) and KL3 (vB_BamM-KL3 or vB_BceZ-CEP511). Results KS5, KS14 and KL3 are myoviruses with the A1 morphotype. The genomes of these phages are between 32317 and 40555 base pairs in length and are predicted to encode between 44 and 52 proteins. These phages have over 50% of their proteins in common with enterobacteria phage P2 and so can be classified as members of the Peduovirinae subfamily and the "P2-like viruses" genus. The BCC phage proteins similar to those encoded by P2 are predominantly structural components involved in virion morphogenesis. As prophages, KS5 and KL3 integrate into an AMP nucleosidase gene and a threonine tRNA gene, respectively. Unlike other P2-like viruses, the KS14 prophage is maintained as a plasmid. The P2 E+E' translational frameshift site is conserved among these three phages and so they are predicted to use frameshifting for expression of two of their tail proteins. The lysBC genes of KS14 and KL3 are similar to those of P2, but in KS5 the organization of these genes suggests that they may have been acquired via horizontal transfer from a phage similar to λ. KS5 contains two sequence elements that are unique among these three phages: an ISBmu 2-like insertion sequence and a reverse transcriptase gene. KL3 encodes an EcoRII-C endonuclease/methylase pair and Vsr endonuclease that are predicted to function during the lytic cycle to cleave non-self DNA, protect the phage genome and repair methylation-induced mutations. Conclusions KS5, KS14 and KL3 are the first BCC-specific phages to be identified as P2-like. As KS14 has previously been shown to be active against Burkholderia cenocepacia in vivo, genomic characterization of these phages is a crucial first step in the development of these and similar phages for clinical use against the BCC.

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    Collection . 2021
    License: CC BY
    Data sources: Datacite
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    figshare
    Collection . 2021
    License: CC BY
    Data sources: Datacite
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      Collection . 2021
      License: CC BY
      Data sources: Datacite
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      Collection . 2021
      License: CC BY
      Data sources: Datacite
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    Simulation of a black-hole binary system evolved by the SpEC code.

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    ZENODO
    Dataset . 2019
    License: CC BY
    Data sources: ZENODO
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    ZENODO
    Dataset . 2019
    License: CC BY
    Data sources: ZENODO
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    ZENODO
    Dataset . 2019
    License: CC BY
    Data sources: Datacite
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    ZENODO
    Dataset . 2019
    License: CC BY
    Data sources: ZENODO
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    ZENODO
    Dataset . 2019
    License: CC BY
    Data sources: ZENODO
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      ZENODO
      Dataset . 2019
      License: CC BY
      Data sources: ZENODO
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      ZENODO
      Dataset . 2019
      License: CC BY
      Data sources: ZENODO
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      ZENODO
      Dataset . 2019
      License: CC BY
      Data sources: Datacite
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      ZENODO
      Dataset . 2019
      License: CC BY
      Data sources: ZENODO
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      ZENODO
      Dataset . 2019
      License: CC BY
      Data sources: ZENODO
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  • Data from Fig 6d. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Unfolded soft drop jet mass distributions for dijet events.

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  • Authors: NA62 Collaboration;

    Upper limits at 90% CL on Branching Ratio of \(K^{+}\rightarrow\pi^{+}X\), and on couplings \(sin^2(\theta)\), vs mass from a search at the NA62 experiment at the CERN SPS. Observed upper limits on branching ratio \(K^{+}\rightarrow\pi^{+}X\) at 90% CL as functions of X mass and lifetime.

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  • Authors: ATLAS Collaboration;

    CERN-LHC. An observation of electroweak $W^{\pm}Z$ production in association with two jets in proton-proton collisions is presented. The data collected by the ATLAS detector at the Large Hadron Collider in 2015 and 2016 at a centre-of-energy of $\sqrt{s}$ = 13TeV are used, corresponding to an integrated luminosity of 36.1 $fb^{-1}$. Events containing three identified leptons, either electrons or muons, and two jets are selected. The electroweak production of $W^{\pm}Z$ bosons in association with two jets is measured with an observed significance of 5.3 standard deviations. A fiducial cross section for electroweak production including interference effects is measured to be $\sigma_{WZjj-EW}$ = 0.57^{+0.14}_{-0.13} (stat.) ^{+0.07}_{-0.06} (syst.) fb. Differential cross section of $W^{\pm}Zjj$ production for several kinematic observables are also measured. Fiducial phase space definition for the measurement: - $p_{\mathrm{T}}$ of electrons and muons from Z0 decays > 15 GeV - $p_{\mathrm{T}}$ of electrons and muons from the $W^{\pm}$ decays > 20 GeV - $|\eta|$ of muons and electrons < 2.5 - Leptons from the Z0 boson are separated by $\Delta R(\ell,\ell) > 0.2$ from each other - Leptons from the Z0 and W bosons are separated by $\Delta R(\ell,\ell) > 0.3$ from each other - |dilepton mass - Z0 mass| < 10 GeV - $m_{\mathrm{T}}$ of $W^{\pm}$ > 30 GeV. - at least 2 jets with opposite $|\eta|$. Jets are particle level jets with anti-kt R=0.4. - $p_{\mathrm{T}}$ of the two jets > 40 GeV - $|\eta|$ of the two jets < 4.5 - the first jet is chosen as the leading $p_{\mathrm{T}}$ jet - the second jet is chosen among the remaining jets as the jet of highest $p_{\mathrm{T}}$ with $|\eta|$ opposite to the first jets - invariant mass of the two jets > 500 GeV - leptons and jets separated by $\Delta R(\ell,jet) > 0.3$ - processes with a b-quark in the initial state are excluded At particle level, the kinematics of final-state prompt electrons and muons is computed including the contributions from final-state radiated photons within a distance in the ($\eta,\phi$) plane of $\Delta R = \sqrt{(\Delta\eta)^2 + (\Delta\phi)^2} = 0.1$ around the direction of the charged lepton. These dressed leptons and the final-state neutrinos that do not originate from hadron or $\tau$ decays are associated with the $W$ and $Z$ boson decay products with an algorithmic approach, called ``resonant shape''. This algorithm is based on the value of an estimator expressing the product of the nominal line shapes of the $W$ and $Z$ resonances $P = \left| \frac{1}{ m^2_{(\ell^+,\ell^-)} - \left(m_Z^{\textrm{PDG}}\right)^2 + i \; \Gamma_Z^{\textrm{PDG}} \; m_Z^{\textrm{PDG}} } \right|^2 \times \; \left| \frac {1} { m^2_{(\ell',\nu_{\ell'})} - \left(m_W^{\textrm{PDG}}\right)^2 + i \; \Gamma_W^{\textrm{PDG}} \; m_W^{\textrm{PDG}} } \right|^2$ where $m_Z^{\textrm{PDG}}$ ($m_W^{\textrm{PDG}}$) and $\Gamma_Z^{\textrm{PDG}}$ ($\Gamma_W^{\textrm{PDG}}$) are the world average mass and total width of the $Z$ ($W$) boson, respectively, as reported by the Particle Data Group \cite{Agashe:2014kda}. The input to the estimator is the invariant mass $m$ of all possible pairs ($\ell^+,\ell^-$) and ($\ell',\nu_{\ell'}$) satisfying the fiducial selection requirements defined in the next paragraph. The final choice of which leptons are assigned to the $W$ or $Z$ bosons corresponds to the configuration exhibiting the highest value of the estimator. Correlation matrix for the unfolded fiducial cross-section.

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  • CERN-LHC. This paper presents a measurement of jet fragmentation functions in 0.49 nb−1 of Pb+Pb collisions and 25 pb−1 of pp collisions at sNN=5.02 TeV collected in 2015 with the ATLAS detector at the LHC. These measurements provide insight into the jet quenching process in the quark-gluon plasma created in the aftermath of ultrarelativistic collisions between two nuclei. The modifications to the jet fragmentation functions are quantified by dividing the measurements in Pb+Pb collisions by baseline measurements in pp collisions. This ratio is studied as a function of the transverse momentum of the jet, the jet rapidity, and the centrality of the collision. In both collision systems, the jet fragmentation functions are measured for jets with transverse momentum between 126 and 398 GeV and with an absolute value of jet rapidity less than 2.1. An enhancement of particles carrying a small fraction of the jet momentum is observed, which increases with centrality and with increasing jet transverse momentum. Yields of particles carrying a very large fraction of the jet momentum are also observed to be enhanced. Between these two enhancements of the fragmentation functions a suppression of particles carrying an intermediate fraction of the jet momentum is observed in Pb+Pb collisions. A small dependence of the modifications on jet rapidity is observed. The ratio of the D(pT) in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.0 < eta < 2.1.

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  • Authors: Weinstabl, Harald; Suhartono, Marcel; Qureshi, Zafar; Lautens, Mark;

    Related Article: Zafar Qureshi, Harald Weinstabl, Marcel Suhartono, Hongqiang Lui, Pierre Thesmar, Mark Lautens|2014|Eur.J.Org.Chem.|2014|4053|doi:10.1002/ejoc.201402218 Related Article: Harald Weinstabl, Marcel Suhartono, Zafar Qureshi and Mark Lautens|2013|Angew.Chem.,Int.Ed.|52|5305|doi:10.1002/anie.201302327

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  • image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/

    Additional file7: Table S18. DNAmeQTL analysis for the loci significantly associated with DNAme-based XCI status calls. See additional files. These loci were independently tested as DNAmeQTLs in females and males, with some columns color coded based on sex (pink female, light blue male). There are also columns with the median and mean DNAme value at the gene’s island for samples with the reference or alternate allele at that loci; these columns are color coded based on whether the allele is in the range to escape from XCI (DNAme<0.01, blue) or in the range to be subject to XCI (DNAme>0.15, orange). There are mean and median columns for both males and females, but only the female columns are color coded based on XCI status. There are boxes around the genes with female median values with one allele in the range to escape XCI and the other allele in the range to be subject to XCI.

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  • Authors: Choing, Stephanie N.; Francis, Aaron J.; Clendenning, Graham; Schuurman, Michael S.; +4 Authors

    An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures. Related Article: Stephanie N. Choing, Aaron J. Francis, Graham Clendenning, Michael S. Schuurman, Roger D. Sommer, Isaac Tamblyn, Walter W. Weare, Tanja Cuk|2015|J.Phys.Chem.C|119|17029|doi:10.1021/acs.jpcc.5b00513

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